Description
This low-mid frequency transducer offers three main points of interest: an extremely linear frequency response and a low harmonic distortion. These characteristics make it suitable for high quality sound reinforcement systems, especially for live applications. Moreover, its versatile design allows it to be used as the low-mid loudspeaker in a two ways system or as an strictly mid-frequency transducer in a three ways system. Beyond its frequency response advantages, this loudspeaker offers more: it takes profit of the improvements achieved in our low frequency-high power transducers. Thus, it incorporates a high quality voice coil and a large magnetic assembly to provide efficient heat dissipation. Thanks to this design concept of strongness, the 12 MI100 reaches a considerable power handling (450 WAES).
● Extremely linear frequency response
● Low harmonic distortion
● 3" edgewound aluminium voice coil with polyimide fiber glass former
● Large magnetic assembly to provide efficient heat dissipation
● Designed for high quality mid-frequency reproduction
Specifications |
|
Nominal diameter | 300 mm 12 in |
Nominal impedance | 8 Ohm |
Minimum impedance | 8 ohm |
Power capacity | 450 W AES |
Program power | 900 W |
Sensitivity | 100 dB 1 W @ 1 m @ 2Π |
Frequency range | 40-4000 Hz |
Voice coil diameter | 77 mm 3 in |
BL factor | 21.6 N / A |
Moving mass | 0.047 kg |
Winding length | 13.5 mm |
Air gap height | 10 mm |
Xdamage pp | 24 mm |
Thiele Small Parameters |
|
Fs | 58 Hz |
Re | 6.3 ohm |
Qms | 5.5 |
Qes | 0.23 |
Qts | 0.22 |
Vas | 64 l |
Cms | 163 µm / N |
Rms | 3.3 kg / s |
Sd | 0.053 m² |
Xmax | 3 mm |
Vd | 159 cm³ |
Le @1 kHz | 1.0 mH |
Construction |
|
Net weight | 7.2 kg 15.8 lb |
Magnet | Ferrite |